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Disturbance in weak measurements and the difference between quantum and classical weak values

机译:弱测量中的干扰和量子与量子之间的差异   经典的弱值

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摘要

The role of measurement induced disturbance in weak measurements is ofcentral importance for the interpretation of the weak value. Uncontrolleddisturbance can interfere with the postselection process and make the weakvalue dependent on the details of the measurement process. Here we develop theconcept of a generalized weak measurement for classical and quantum mechanics.The two cases appear remarkably similar, but we point out some importantdifferences. A priori it is not clear what the correct notion of disturbanceshould be in the context of weak measurements. We consider three differentnotions and get three different results: (1) For a `strong' definition ofdisturbance, we find that weak measurements are disturbing. (2) For a weakerdefinition we find that a general class of weak measurements arenon-disturbing, but that one gets weak values which depend on the measurementprocess. (3) Finally, with respect to an operational definition of the `degreeof disturbance', we find that the AAV weak measurements are the leastdisturbing, but that the disturbance is always non-zero.
机译:测量引起的干扰在弱测量中的作用对于弱值的解释至关重要。不受控制的干扰会干扰后选过程,并使弱值取决于测量过程的细节。在这里,我们为经典力学和量子力学开发了广义弱测量的概念。这两种情况看起来非常相似,但我们指出了一些重要的区别。先验地还不清楚在弱测量的情况下,正确的干扰概念应该是什么。我们考虑了三个不同的概念并获得了三个不同的结果:(1)对于“强”的扰动定义,我们发现弱测量值令人不安。 (2)对于较弱的定义,我们发现一类普通的弱测量是无干扰的,但得出的弱值取决于测量过程。 (3)最后,关于“扰动度”的操作定义,我们发现AAV弱测量值是最小的扰动,但扰动总是非零的。

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    Ipsen, Asger C.;

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  • 年度 2015
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  • 正文语种 {"code":"en","name":"English","id":9}
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